TY - JOUR
T1 - Calculation of bulk modulus and its pressure derivatives from vibrational frequencies and mode Gruneisen parameters
T2 - solids with cubic symmetry or one nearest-neighbor distance
AU - Hofmeister, A. M.
PY - 1991
Y1 - 1991
N2 - The bulk modulus KT can be related to structural parameters and to the sum of the squares of the vibrational frequencies, Σvi2, for N-atom crystals of cubic symmetry or for any symmetry that contains only one nearest-neighbor distance. Required assumptions are the existence of (1) electrostatic forces exclusively between atoms at equivalent positions in the primitive unit cell, (2) pair-wise central repulsive potentials between all other atoms, and (3) rigid ions. Including pressure in the derivation requires a more stringent version of point 2, namely, (4) that the structure scales isotropically upon compression. This leads to structurally independent formulas for the pressure derivatives of bulk modulus at 1 atm; the only variables are KT and sums involving vi2 and the first or second pressurderivative of vi, i.e., the mode Gruneisen parameters. Implicit in all equations is the independence of the sums on wave vector. Thus, knowledge of zone center phonons (mostly infrared and Raman bands) is sufficient to calculate elastic properties. -from Author
AB - The bulk modulus KT can be related to structural parameters and to the sum of the squares of the vibrational frequencies, Σvi2, for N-atom crystals of cubic symmetry or for any symmetry that contains only one nearest-neighbor distance. Required assumptions are the existence of (1) electrostatic forces exclusively between atoms at equivalent positions in the primitive unit cell, (2) pair-wise central repulsive potentials between all other atoms, and (3) rigid ions. Including pressure in the derivation requires a more stringent version of point 2, namely, (4) that the structure scales isotropically upon compression. This leads to structurally independent formulas for the pressure derivatives of bulk modulus at 1 atm; the only variables are KT and sums involving vi2 and the first or second pressurderivative of vi, i.e., the mode Gruneisen parameters. Implicit in all equations is the independence of the sums on wave vector. Thus, knowledge of zone center phonons (mostly infrared and Raman bands) is sufficient to calculate elastic properties. -from Author
UR - https://www.scopus.com/pages/publications/0026278265
U2 - 10.1029/91jb01381
DO - 10.1029/91jb01381
M3 - Article
AN - SCOPUS:0026278265
SN - 0148-0227
VL - 96
SP - 16,181-16,203
JO - Journal of Geophysical Research: Biogeosciences
JF - Journal of Geophysical Research: Biogeosciences
IS - B10
ER -